“…The underlying phase transition is a first order transition where phase equilibrium exists and the nucleation process has been intensely studied [42][43][44][45][46][47][48][49][50][51][52][53][54][55][56]. The most widely used concept, the Classical Nucleation Theory (CNT), attempts to describe this complex process by treating the nuclei as compact spheres that grow if their size exceeds a critical value [42][43][44]. However, experiments on hard sphere colloidal systems [48,49,52] differ from the predictions of critical nucleation theory and the CNT calculation underestimates the nucleation rate by many orders of magnitude [57].…”
Abstract. We use super-paramagnetic colloidal particles confined by gravitation to a flat water-air interface as a model system to study the non-equilibrium liquid-solid phase transition in two dimensions. The system temperature is adjustable by changing the strength of an external magnetic field perpendicular to the water-air interface. Increasing the magnetic field on a timescale of milliseconds quenches the liquid to a strongly super-cooled state. If the system is cooled down out of equilibrium the solidification differs drastically from the equilibrium melting and freezing scenario as no hexatic phase is observable. The system solidifies to a polycrystalline structure with many grains of different orientations. Since the local closed packed order in two dimensions is sixfold, in both the fluid and the crystalline state, sensitive measures have to be developed. In the present manuscript we compare different methods to identify crystalline cluster locally and motivate the threshold values. Those are chosen in comparison with the isotropic fluid on one hand and large mono-crystals in thermal equilibrium on the other hand. With the given criteria for crystalline cluster the cluster are found not to be circular and fractal dimensions of the grains are given.
“…The underlying phase transition is a first order transition where phase equilibrium exists and the nucleation process has been intensely studied [42][43][44][45][46][47][48][49][50][51][52][53][54][55][56]. The most widely used concept, the Classical Nucleation Theory (CNT), attempts to describe this complex process by treating the nuclei as compact spheres that grow if their size exceeds a critical value [42][43][44]. However, experiments on hard sphere colloidal systems [48,49,52] differ from the predictions of critical nucleation theory and the CNT calculation underestimates the nucleation rate by many orders of magnitude [57].…”
Abstract. We use super-paramagnetic colloidal particles confined by gravitation to a flat water-air interface as a model system to study the non-equilibrium liquid-solid phase transition in two dimensions. The system temperature is adjustable by changing the strength of an external magnetic field perpendicular to the water-air interface. Increasing the magnetic field on a timescale of milliseconds quenches the liquid to a strongly super-cooled state. If the system is cooled down out of equilibrium the solidification differs drastically from the equilibrium melting and freezing scenario as no hexatic phase is observable. The system solidifies to a polycrystalline structure with many grains of different orientations. Since the local closed packed order in two dimensions is sixfold, in both the fluid and the crystalline state, sensitive measures have to be developed. In the present manuscript we compare different methods to identify crystalline cluster locally and motivate the threshold values. Those are chosen in comparison with the isotropic fluid on one hand and large mono-crystals in thermal equilibrium on the other hand. With the given criteria for crystalline cluster the cluster are found not to be circular and fractal dimensions of the grains are given.
“…That is, for large i, ⍜ should approach A 1 ␥ ϱ /(kT), where A 1 i 2/3 is the surface area of a spherical droplet containing i monomers at the bulk liquid density, and ␥ ϱ is the surface tension of a planar interface. In order that this should be consistent with the ⍜ chosen by Kiang et al 15 and Hamill et al, 16 i.e., with the low temperature equation of state, ⍜ has to be size dependent. Dillmann and Meier wrote…”
Section: History Of the Fisher Modelmentioning
confidence: 49%
“…͑5͒ and showed that it was close to the value required by Fisher's analysis of critical exponents.͔ The next step was to use the model to study nucleation phenomena away from the critical point. This was carried out by Kiang et al 15 and later by Hamill et al 16 In these treatments, the parameter ⌰ was chosen such that the low temperature imperfect properties of the vapor were reproduced. This was equivalent to introducing a size independent microscopic surface energy and relating it to the low temperature second virial coefficient of the vapor.…”
“…In clouds, ice appears in a variety of forms, shapes, depending on the formation mechanism and the atmospheric conditions 22,51,67,68 . The cloud inner structure, content, temperature, life time, .. can be studied.…”
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